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Physica A Statistical Mechanics and its Applications

Spin-glass in low dimensions and the Migdal-Kadanoff approximation

Evaldo M. F. Curado, J.L. Meunier

Published Mar 1, 1988• 25 citations
Publisher
DOI
10.1016/0378-4371(88)90212-9

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We have studied the random-axis magnet with infinite anisotropy by three methods: Cayley-tree approximation, Migdal-Kadanoff renormalization group (MKRG), and Imry-Ma scaling. In the Cayley-tree approximation, by an examination of susceptibilities, it is shown that there exists a competition between the coordination number z and the number of components n of the spins which leads to either ferromagnetic or spin-glass order. Using the MKRG at very low temperature we map out approximately the regimes of the ferromagnetic, spin-glass, and disordered phases as a function of n and the spatial dimension, d. The Imry-Ma arguments are made as an additional method for obtaining information on the critical dimension. Comparisons of these results with the previous literature are made.
We discuss the zero-temperature behavior of the transverse Ising spin-glass ($\ifmmode\pm\else\textpm\fi{}{J}_{0}$) model. The ddd-dimensional quantum model is shown to be equivalent to a classical (d+1d+1d+1)-dimensional Ising spin glass with correlated disorder. A renormalization-group treatment of the one-dimensional quantum model indicates the existence of a spin-glass phase. The Migdal-Kadanoff approximation is used to obtain the phase diagram of the quantum spin glass in two dimensions.